# MacRobert E function

(Redirected from MacRobert E-function)

In mathematics, the E-function was introduced by Thomas Murray MacRobert (1937–38) to extend the generalized hypergeometric series pFq(·) to the case p > q + 1. The underlying objective was to define a very general function that includes as particular cases the majority of the special functions known until then. However, this function had no great impact on the literature as it can always be expressed in terms of the Meijer G-function, while the opposite is not true, so that the G-function is of a still more general nature.

## Definition

There are several ways to define the MacRobert E-function; the following definition is in terms of the generalized hypergeometric function:

• when pq and x ≠ 0, or p = q + 1 and |x| > 1:
$E \!\left( \left. \begin{matrix} \mathbf{a_p} \\ \mathbf{b_q} \end{matrix} \; \right| \, x \right) = \frac{\prod_{j=1}^{p} \Gamma (a_j)} {\prod_{j=1}^{q} \Gamma (b_j)} \;_{p}F_{q} \!\left( \left. \begin{matrix} \mathbf{a_p} \\ \mathbf{b_q} \end{matrix} \; \right| \, -x^{-1} \right)$
• when pq + 2, or p = q + 1 and |x| < 1:
$E \!\left( \left. \begin{matrix} \mathbf{a_p} \\ \mathbf{b_q} \end{matrix} \; \right| \, x \right) = \sum_{h=1}^{p} \frac{\prod_{j=1}^{p} \Gamma (a_j - a_h)^*} {\prod_{j=1}^{q} \Gamma (b_j - a_h)} \Gamma (a_h) \; x^{a_h} \;_{q+1}F_{p-1} \!\left( \left. \begin{matrix} a_h, 1 + a_h - b_1, \dots, 1 + a_h - b_q \\ 1 + a_h - a_1, \dots, *, \dots, 1 + a_h - a_p \end{matrix} \; \right| \, (-1)^{p-q} \;x \right).$

The asterisks here remind us to ignore the contribution with index j = h as follows: In the product this amounts to replacing Γ(0) with 1, and in the argument of the hypergeometric function this amounts to shortening the vector length from p to p − 1. Evidently, this definition covers all values of p and q.

## Relationship with the Meijer G-function

The MacRobert E-function can always be expressed in terms of the Meijer G-function:

$E \!\left( \left. \begin{matrix} \mathbf{a_p} \\ \mathbf{b_q} \end{matrix} \; \right| \, x \right) = G_{q+1,\,p}^{\,p,\,1} \!\left( \left. \begin{matrix} 1, \mathbf{b_q} \\ \mathbf{a_p} \end{matrix} \; \right| \, x \right)$

where the parameter values are unrestricted, i.e. this relation holds without exception.

## References

• Andrews, L. C. (1985). Special Functions for Engineers and Applied Mathematicians. New York: MacMillan. ISBN 0-02-948650-5.
• Erdélyi, A.; Magnus, W.; Oberhettinger, F. & Tricomi, F. G. (1953). Higher Transcendental Functions (PDF). Vol. 1. New York: McGraw–Hill. (see § 5.2, "Definition of the E-Function", p. 203)
• Gradshteyn, Izrail' Solomonovich & Ryzhik, Iosif Moiseevich (1971). Tablitsy integralov, summ, ryadov i proizvedeniy [Tables of integrals, sums, series and products] (in Russian) (5th ed.). Moscow: Nauka. (see Chapter 9.4)
• MacRobert, T. M. (1937–38). "Induction proofs of the relations between certain asymptotic expansions and corresponding generalised hypergeometric series". Proc. Roy. Soc. Edinburgh 58: 1–13. JFM 64.0337.01.
• MacRobert, T. M. (1962). "Barnes integrals as a sum of E-functions". Mathematische Annalen 147 (3): 240–243. doi:10.1007/bf01470741. Zbl 0100.28601.